Before discussing the main results, let us mention the predicted values for the different exponents.
The first three scaling relations enable us to express \(\delta \) , \(\eta \)  and \(\zeta \)  in terms of \(\xi _1\)  only. This is particularly interesting since \(\xi _1\)  is measurable in terms of the scaling limit of interfaces at criticality.
The relations R6 and R7 link \(\alpha \) , \(\nu \)  and \(\iota \) . This is again very useful since it was noted in the previous section how \(\iota \)  can be obtained from the understanding of the scaling limit of interfaces. An alternative approach to computing these three exponents would be to first obtain \(\alpha \) , which may perhaps be derived using exact integrability of the random-cluster model, see [1]} and Section REF  for more details.
Finally, R4 and R5 express \(\beta \)  and \(\gamma \)  in terms of \(\xi _1\)  and \(\nu \) , so that one can obtain all the exponents from \(\xi _1\)  and \(\iota \)  (or \(\alpha \) ).
